Journal of Water Resource and Protection, 2012, 4, 346-353 http://dx.doi.org/10.4236/jwarp.2012.46039 Published Online June 2012 (http://www.SciRP.org/journal/jwarp)

Geoelectric Sounding for the Determination of Aquifer Transmissivity in Parts of Bayelsa State,

South South Nigeria

Kenneth S. Okiongbo1*, Ebifuro Odubo2 1Department of Geology & Physics, Niger Delta University, Wilberforce Island, Nigeria

2Department of Geography and Environmental Management, Niger Delta University, Wilberforce Island, Nigeria Email: *okenlani@yahoo.com

Received March 12, 2012; revised April 6, 2012; accepted May 1, 2012

ABSTRACT

The application of geophysical methods in combination with pumping tests provides a cost-effective and efficient al-ternative to estimate aquifer parameters. In this study, nineteen Schlumberger vertical electrical soundings (VES) were occupied in parts of Bayelsa State using a maximum current electrode separation ranging beweeen 300 - 400 m with the aim of estimating the transmissivity of the alluvial aquifer in areas where no pumping test has been carried out. Four of the soundings were carried out near existing boreholes in which pumping test had been carried out. The VES data ob-tained was interpreted, and layer parameters such as true resistivities and thickness were determined. The geoelectric parameters were used to generate the Dar Zarrouk parameters. Correlating the Dar Zarrouk parameter (e.g longitudinal unit conductance) with transmissivity derived from pumping test data, a constant was found which translate longitudinal unit conductance to transmissivity in a hydrogeological setting where effective porosity is the primary control on resis-tivity and hydraulic conductivity. Transmissivity determined from the pumping test data range between 1634.0 - 5292.0 m2/day while transmissivity values estimated from the longitudinal unit conductance (Lc) range between 721 - 8991 m2/day. The transmissivity estimated from the pumping test (Tp) data and transmissivity estimated from the longitudinal conductance (Lc) on comparison show excellent correlation (R2 = 0.92). The high transmissivity values agree with the geology of the Benin Formation (Coastal Plain sands) consisting of fine-medium-coarse sands. The results give a useful first approximation of the transmissivity and could be used to site exploratory boreholes. Keywords: Aquifer; Longitudinal Conductance; Transmissivity; Dar Zarrouk Parameters; Geoelectric Parameters;

Yenagoa

1. Introduction

The evaluation of hydraulic properties of subsurface aq-uifers is an important task in groundwater resources as-sessment and development. This is because these proper-ties are important in determining the natural flow of wa-ter through an aquifer and its response to fluid extraction [1]. Besides, they are useful parameters for groundwater protection and prediction of contaminant transport [2]. Several methods are available in Groundwater Hydrol-ogy for evaluation and estimation of these aquifer char-acteristics. The most commonly used methods involve conducting pumping test on existing or newly drilled wells followed by analysis and interpretation of the pumping test data. However, such tests are both capital and labour intensive requiring several boreholes, many operatives, and a considerable amount of equipment. Besides, the

pumping test method yields results appropriate only to a small section of the aquifer.

An alternative approach for estimating aquifer charac-teristics is the use of surface geoelectrical methods. The surface geoelectrical method especially the Vertical Electrical Sounding (VES) method of geophysical inves-tigation is a non-invasive, relatively cheap and quantita-tive evaluation technique used for locating sites/depths for groundwater exploitation. Besides, it is used as an effective tool for ascertaining the subsurface geological framework of an area [3-5], and thus being used rou-tinely for aquifer zone delineation and evaluation of the geophysical character of the aquifer. Since a correlation between hydraulic and electrical properties is possible, as both properties are related to the pore space structure and heterogeneity [6-7], the integration of aquifer parameters calculated from boreholes and surface resistivity pa-rameters extracted from surface resistivity measurements *Corresponding author.

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K. S. OKIONGBO, E. ODUBO 347

is an effective method in estimating aquifer properties. In this study, this approach has been utilized in order to estimate aquifer transmissivity in numerous locations providing effective and inexpensive characterization of the study area aquifer system.

2. Geology and Hydrogeology of the Study Area

The study area lies between latitudes 4˚48' and 5˚08' north and Longitudes 6˚06' and 6˚30' east, South South Nigeria (Figure 1). It is within the Tropical Equatorial climate. There are two major climatic seasons in the area,

the wet season from April to October and the dry season from November to March. Average annual rainfall is about 3000 mm [8] and this serves as the major source of groundwater recharge. This ensures a large volume of water input into the environment. There are a number of perennial streams and rivers in the area of study. They all form a network which empties to the Atlantic Ocean. As a result, most of the terrain is marshy and in some cases form beaches. The topography is invariably gentle. Plant type is generally mangrove except in the mainland areas where large areas are covered with oil palm and large trees.

A

A1

Figure 1. Map of study area showing sounding and Borehole (BH) points.

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K. S. OKIONGBO, E. ODUBO 348

The study area is within the lower section of the upper

flood plain deposits of the subearial Niger Delta [9]. The deposits are characterized by pebbles and coarse to fine sands with intercalations of silt, mud and clay in places. A variety of depositional environments (point bars, chan- nel fills, natural levees and splay deposits, backswamps, ox-bow fills and palludal deposits) are typical [10]. The thickness of these Quaternary sediments does not exceed 120 m and it is predominantly unconfined. The specific capacities recorded from different areas within this for-mation vary from 6700 lit/hr/m to 13,000 lit/hr/m [11]. Underlying these Quaternary sediments is the Benin Formation which is about 2100 m thick on the average [10]. The formation represents the subsurface continental megafacies of the Niger Deltaic sequence (Table 1). It is essentially fluvial in origin and comprises of unconsoli-dated, massive, and porous freshwater bearing sands with localized shale interbeds. All the aquifers in the delta region are located within this lithounit. However, only the upper 200 m has been penetrated by boreholes in the study area. The age ranges from Miocene to Recent. The underlying paralic Agbada Formation, varies in thickness from 300 to 4500 m. The formation consists predomi-nantly of unconsolidated pebbles, and very coarse to fine grained sand units with surbodinate shale beds. Syntec-tonic growth faults and rollover anticlinal structures are characteristic. These commonly form the major traps for oil and gas in the delta. Age ranges from Oligocene to Recent.

3. Materials and Methods

3.1. Mathematical Formulation

The combination of thickness and resistivity into single variables other words known as Dar Zarrouk parameters are used as a basis for the evaluation of aquifer properties [12-13]. The concept of Dar Zarrouk parameters were first introduced by [14] to explain the problem of non-uniqueness in the interpretation of resistivity depth sounding curves. Analytical relations between aquifer transmissivity and Dar Zarrouk parameters have been developed and various data sets tested [12,15-16]. The Dar Zarrouk parameters consist of the transverse resis-tance (RT) and longitudinal conductance (Lc). For a hori-zontal, homogeneous, and isotropic layer, the transverse resistance RT (Ωm2) is defined as:

TR h (1)

and the longitudinal conductance Lc (mho) is defined as:

CL h (2)

where h is the thickness of the layer (in metres) and ρ is the electrical resistivity of the layer in ohm-metres. In such a simple horizontal layer model, Niwas and Singhal.

[12] established an analytical relationship between transmissivity and the Dar Zarrouk parameters based on the analogy between Darcy’s law of groundwater flow and Ohm’s law of current flow as follows:

TT K R

CT K L

(3)

(4)

where T is the transmissivity (m2/d) defined as the prod-uct of aquifer hydraulic conductivity (K) and thickness (h), i.e.

T Kh (5) RT and Lc are the transverse resistance and longitudinal

conductance respectively. Henriet, [17] observed that hy-draulic conductivity of clayey sediment could be linked to electrical resistivity through the concept of clay con-tent and that high clay contents generally correspond with low resistivities and hydraulic conductivity. In other words, in a clay-rich aquifer, a linear relationship exists between hydraulic conductivity and resistivity [12,18]. Therefore,

K 1C (6)

Frohlich and Kelly, [19] reported that in an uncon-solidated, sandy, clay-free aquifer, a direct relationship exists between hydraulic conductivity and porosity (K α Φ), while an inverse relationship exists between porosity and resistivity (Φ α 1/ρ). Therefore,

K 2C (7)

where C1 and C2 are constants. Substituting Equation (6) into (3), and Equation (7) into (4) gives Table 1. Stratigraphic column of the Niger Delta (after Al-len, 1965).

Geologic Unit Lithology Age

Alluvium (general) Gravel, sand, clay, silt

Freshwater backswamp, meander belt

Sand, clay, some silt gravel

Mangrove and salt water/backswamps

Medium-fine sands, clay and some silt

Quaternary

Active/abandoned beach ridges

Sand, clay, and some silt

Sombreiro-Warri deltaic plain

Sand, clay, and some silt

Benin Formation (Coastal Plain sand)

Coarse to medium sand with subordinate silt and clay lenses

Miocene

Agbada Formation Mixture of sand, clay and silt

Eocene

Akata Formation Clay Paleocene

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K. S. OKIONGBO, E. ODUBO 349

1TT R C

2CT L C

(8)

(9)

It implies therefore that in clay free sandy hydro-geological environments, Kρ can be considered constant; and in clay—rich environments K would remain constant. A presumption in these theoretical relations is that changes in resistivity and hydraulic conductivity across the aquifer are controlled exclusively by one fac-tor at a time, either variations in effective porosity (Equa-tion (7)) or changes in clay content (Equation (6)). Aside, the electrical conductivity of the groundwater is pre-sumed not to vary significantly throughout the aquifer as this would also affect the measured resistivity [12].

Frohlich and Kelly, [18] observed that the transverse resistance is the dominant parameter for a layer when the electrical current tends to flow perpendicular to the bed-ding and therefore controls the shape of a K-shaped

sounding curve i.e. where the middle of the three layers is of higher resistivity. Besides, when the electrical cur-rent flows parallel to the bedding, as in an H-type curve, the longitudinal conductance is the dominant parameter (Figure 2). [19] therefore suggested that depending on the geological conditions, transmissivity can be directly related to the transverse resistance or to the longitudinal conductance: the transverse resistance when clay content controls hydraulic conductivity (K-shaped) and longitu-dinal conductance when effective porosity is the control-ling factor (H-shaped curve). Since transmissivity and the Dar Zarrouk parameters are bulk parameters, esti-mates of the appropriate constant (either C1 or C2) can be calculated by relating aquifer pumping test results and surface resistivity measurements at a few points in the aquifer. Transmissivity variations over the rest of the aquifer can then be easily determined from additional surface resistivity measurements.

Figure 2. Resistivity soundings and interpretation at the four sites with transmissivity values.

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3.2. Data Acquisition and Interpretation

The locations of the sounding points are shown in Figure 1. Vertical Electric Sounding using the Schlumberger electrode configuration was carried out by applying cur-rent to the ground through two electrodes (A and B) and then measuring the resultant potential difference (∆V) between the potential electrodes (M and N). The center point of the electrode array remains fixed but the spac-ings of the electrodes was increased so as to obtain in-formation about the stratification of the ground [20]. The Schlumberger data are mostly taken in overlapping seg-ments because at each step of AB spacing, the signals of the resistivity meter become weaker. Therefore, MN spacing was enlarged and two values for the same AB/2 were measured, one for the short and one for the long MN spacing.

The Schlumberger configuration was employed not only because it is faster and less likely to be influenced by lateral variations but also because it requires a lower number of operators. Because of extensive dense foresta-tion and swampy terrain, soundings were carried out along existing foot paths or roads. A total of 19 VES sites were occupied. Array spread for current electrode spacing range between 300 to 400 m. The ZTI 1500 re-sistivity meter was used in this investigation.

Apparent resistivity values were determined by taking the product of the resistance as measured by the Terram-eter and the geometrical factor, a parameter which is de-pendent on the potential and current electrode spacings.

The data obtained was later subjected to computer as-sisted iterative interpretation using a 1-D inversion tech-nique software (1X1D, Interpex, USA). This programme was used to perform quantitative analysis and interpreta-tion of the field curves. The software requires that the operator introduce the number, thickness, and resistivi-ties of the subsurface layers. The theoretical curve for the initial input parameters is compared with the measured data. The starting model and its corresponding resistivity are transformed, refined or modified by the programme to obtain a best fit relation to the field data. The method of iteration was performed until the fitting error between field data and synthetic model curve became least and constant. Thus, the software yields the number, thickness and resistivity of the various layers. Borehole (BH) data was used to minimize the choice of equivalent models, by fixing thicknesses and depths to certain levels and allowing adjustment of resistivity. Correlation between VES interpretation at station 2 and borehole lithology determines the electrical characteristics of the rock units with depth (Figure 3). Figure 2 shows VES curves at four sites. Four soundings were made at the sites of ex-isting boreholes. The respective VES stations are 02, 04, 08 and 11. Pumping test was also performed on these wells, which involve the measurement of the rise and fall of water level with respect to time. The tests were per-formed using submersible pumps and observations were made in the same wells. The data obtained was analyzed using Jacob Straight line method to obtain the transmis-sivity of the aquifer at these locations. The locations of the pumping wells are shown in Figure 1.

0

10

20

30

40

50

60

70

80

90

126m ??

230m

57m 31m

Depth (m) VES02

Top Soil

Cla

0

10

20

30

40

50

60

70

80

90

Litholog

y and Clayey sand

Fine‐medium Coarse Sand

? ? ? ?

‐‐ ‐ ‐‐‐‐‐‐‐‐‐

Fine‐medium

Coarse Sand

Top Soil

Clay

LEGEND

Clayey Sand

‐‐‐‐‐‐‐‐‐ ‐‐‐‐‐‐‐‐‐ ‐‐‐‐‐‐‐‐‐ ‐‐‐‐‐‐‐‐‐ ‐‐‐‐‐‐‐‐‐ ‐‐‐‐‐‐‐‐‐ ‐‐‐‐‐‐‐‐‐

100

100

‐‐ ‐ ‐‐‐‐‐‐‐‐‐ ‐‐ ‐ ‐‐‐‐‐‐‐‐‐ ‐‐ ‐ ‐‐‐‐‐‐‐‐‐

Figure 3. Correlation of VES 02 and lithology.

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K. S. OKIONGBO, E. ODUBO 351

The general shape of the resistivity curves (Figure 2)

suggests that the longitudinal conductance can be con-sidered as the dominant Dar Zarrouk parameter. Since the longitudinal conductance is the dominant parameter, Equation (8) was used to calculate the transmissivity. From the interpretation of the resistivity data, it was pos-sible to compute, for every VES station, the longitudinal unit conductance. Therefore, using data from the four locations where both transmissivity and longitudinal conductance data were available, a linear regression was taken between transmissivity and longitudinal conduc-tance (Figure 4). A significant direct relation is illus-trated by the data, giving a value of 2,067,900 Ω–1·m–1 for C2. Comparison of transmissivity estimated from pump-ing test data and transmissivity estimated from the longi-tudinal conductance (Figure 5) show excellent correla-tion (R2 = 0.92). Using the longitudinal unit conductance from the resistivity survey, the transmissivity at each of the VES sites was calculated. The transmissivity distri-bution in the entire area was therefore estimated (Figure 6).

Figure 4. Longitudinal conductance and transmissivity at four sites within the study area.

Figure 5. Correlation of measured and modeled transmis-sivity in the study area.

6.1 6.15 6.2 6.25 6.3 6.35 6.44.45

4.5

4.55

4.6

4.65

4.7

4.75

4.8

4.85

4.9

4.95

5

Longitude (degree)

Lat

itud

e (d

egre

e)

Figure 6. Transmissvity distribution in the study area esti-mated from the Dar Zarrouk transmissivity method.

4. Results and Discussion

Aquifer geoelectric parameters are presented in Table 2. Also shown in Table 2 are both measured and modeled transmissivity values determined from pumping test analysis using Jacob’s straight line method and those estimated using the Dar Zarrouk transmissivity method outlined in this study. Transmissivity distribution in the entire area is shown in Figure 6. Aquifer thickness is highly variable in the study area (Table 1), ranging be-tween 11 m in the vicinity of VES 9 and 98.0 m in the vicinity of VES 2.

The lithology as inferred from litholog is fine-me- dium-coarse sand (Figure 3). The resistivity of the aqui- ferous layer range between 230 - 2868.2 Ωm with an av-erage of 1014.7 Ωm. The transmissivity values are high over the entire area implying good groundwater potential. Measured transmissivity values range between 1634.0 - 5292.0 m2/day with an average of 2987.0 m2/day, while calculated transmissivity values range between 721.0 - 8991.0 m2/day with an average of about 3339.4 m2/day (Table 2).

Computed transmissivity values were plotted against transmissivity values determined from the pumping test data obtained in the same location (Figure 5). The re-gression line fitted to these data indicated a fairly good relation giving R2 = 0.92. The high transmissivity values

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K. S. OKIONGBO, E. ODUBO 352

Table 2. Aquifer geoelctric parameters with measured and modeled Transmissivity values.

VES No

Thickness (m)

Resistivity (Ωm)

Longitudinal Unit Conductance (Ω–1·m–1)

Measured Transmissivity (m2/day)

Modelled Transmissivity (m2/day )

1 40.8 2117.4 0.000472 976

2 97.6 230.0 0.004347 5292 8991

4 13.0 845.0 0.001183 1634 2447

5 47.5 509.5 0.001963 4059

6 27.6 628.7 0.001591 3290

7 17.6 828.6 0.001207 2496

8 43.8 1964.0 0.000509 1872 1053

9 10.7 506.3 0.001975 4084

10 45.0 1214.1 0.000824 1703

11 47.2 634.6 0.001575 3150 3262

12 25.6 663.5 0.001507 3117

13 81.2 376.1 0.002659 5498

15 22.8 293.0 0.003410 7052

18 21.1 2868.2 0.000349 721

19 51.8 1540.8 0.000649 1342

are consistent with the finding that the aquifer is com-posed of unconsolidtated fine-medium-coarse sands. Bore-holes and wells located in the area are highly productive. The estimated transmissivity values of the quaternary alluvial sediments show a wide variation presumably due to the inhomogeneity of the sedimentary formation.

5. Conclusion

Drilling of wells to determine aquifer hydraulic parame-ters is often prohibitively expensive, thus Dar Zarrouk transmissivity technique outlined in this study in deter-mining the aquifer transmissivity from VES is a cost ef-fective alternative. The advantage of using Dar Zarrouk parameters to estimate transmissivity is that the non- uniqueness of interpreting resistivity data is minimized. The results give a useful first approximation of the transmissivity variation and could be used to site ex-ploratory boreholes. Transmissivity values derived from analyzing pumping test data range from 1634.0 - 5292.0 m2/day while estimated transmissivity values range from 721.0 m2/day to 8991.0 m2/day. The correlation coeffi-cient i.e. R2 = 0.92. The close agreement between esti-mated transmissivity values from analysis of vertical electric sounding data and transmissivity values calcu-lated from pumping test data attests to the validity of the method. The high transmissivity values recorded over most parts of the area also agree with the geology of the Benin Formation (Coastal Plain Sands) consisting of fine-medium-coarse grained sands.

6. Acknowledgements

We are grateful to Mr Eleazer Ogulu for assisting in car-rying out the pumping test and Dr Ebisomu Agedeh, for allowing us to use his borehole for the pumping test. Special thanks to Mr Franklin Akali for helping in ac-quiring the VES data.

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